Normalized frequency (unit)

☆ Save On Wikipedia ↗

In digital signal processing (DSP), a normalized frequency is a ratio of a variable frequency ( f {\displaystyle f} {\displaystyle f}) and a constant frequency associated with a system (such as a sampling rate, f s {\displaystyle f_{s}} {\displaystyle f_{s}}). Some software applications require normalized inputs and produce normalized outputs, which can be re-scaled to physical units when necessary. Mathematical derivations are usually done in normalized units, relevant to a wide range of applications.

Examples of normalization

A typical choice of characteristic frequency is the sampling rate ( f s {\displaystyle f_{s}} {\displaystyle f_{s}}) that is used to create the digital signal from a continuous one. The normalized quantity, f ′ = f f s , {\displaystyle f'={\tfrac {f}{f_{s}}},} {\displaystyle f'={\tfrac {f}{f_{s}}},} has the unit cycle per sample regardless of whether the original signal is a function of time or distance. For example, when f {\displaystyle f} {\displaystyle f} is expressed in Hz (cycles per second), f s {\displaystyle f_{s}} {\displaystyle f_{s}} is expressed in samples per second.[1]

Some programs (such as MATLAB toolboxes) that design filters with real-valued coefficients prefer the Nyquist frequency ( f s / 2 ) {\displaystyle (f_{s}/2)} {\displaystyle (f_{s}/2)} as the frequency reference, which changes the numeric range that represents frequencies of interest from [ 0 , 1 2 ] {\displaystyle \left[0,{\tfrac {1}{2}}\right]} {\displaystyle \left[0,{\tfrac {1}{2}}\right]} cycle/sample to [ 0 , 1 ] {\displaystyle [0,1]} {\displaystyle [0,1]} half-cycle/sample. Therefore, the normalized frequency unit is important when converting normalized results into physical units.

Example of plotting samples of a frequency distribution in the unit "bins", which are integer values. A scale factor of 0.7812 converts a bin number into the corresponding physical unit (hertz).

A common practice is to sample the frequency spectrum of the sampled data at frequency intervals of f s N , {\displaystyle {\tfrac {f_{s}}{N}},} {\displaystyle {\tfrac {f_{s}}{N}},} for some arbitrary integer N {\displaystyle N} {\displaystyle N} (see § Sampling the DTFT). The samples (sometimes called frequency bins) are numbered consecutively, corresponding to a frequency normalization by f s N . {\displaystyle {\tfrac {f_{s}}{N}}.} {\displaystyle {\tfrac {f_{s}}{N}}.}[2]: p.56 eq.(16) [3] The normalized Nyquist frequency is N 2 {\displaystyle {\tfrac {N}{2}}} {\displaystyle {\tfrac {N}{2}}} with the unit ⁠1/N⁠th cycle/sample.

Angular frequency, denoted by ω {\displaystyle \omega } {\displaystyle \omega } and with the unit radians per second, can be similarly normalized. When ω {\displaystyle \omega } {\displaystyle \omega } is normalized with reference to the sampling rate as ω ′ = ω f s , {\displaystyle \omega '={\tfrac {\omega }{f_{s}}},} {\displaystyle \omega '={\tfrac {\omega }{f_{s}}},} the normalized Nyquist angular frequency is π radians/sample.

The following table shows examples of normalized frequency for f = 1 {\displaystyle f=1} {\displaystyle f=1} kHz, f s = 44100 {\displaystyle f_{s}=44100} {\displaystyle f_{s}=44100} samples/second (often denoted by 44.1 kHz), and 4 normalization conventions:

Quantity Numeric range Calculation Reverse
f ′ = f f s {\displaystyle f'={\tfrac {f}{f_{s}}}} {\displaystyle f'={\tfrac {f}{f_{s}}}}   [0, ⁠1/2⁠] cycle/sample 1000 / 44100 = 0.02268 f = f ′ ⋅ f s {\displaystyle f=f'\cdot f_{s}} {\displaystyle f=f'\cdot f_{s}}
f ′ = f f s / 2 {\displaystyle f'={\tfrac {f}{f_{s}/2}}} {\displaystyle f'={\tfrac {f}{f_{s}/2}}}   [0, 1] half-cycle/sample 1000 / 22050 = 0.04535 f = f ′ ⋅ f s 2 {\displaystyle f=f'\cdot {\tfrac {f_{s}}{2}}} {\displaystyle f=f'\cdot {\tfrac {f_{s}}{2}}}
f ′ = f f s / N {\displaystyle f'={\tfrac {f}{f_{s}/N}}} {\displaystyle f'={\tfrac {f}{f_{s}/N}}}   [0, ⁠N/2⁠] bins 1000 × N / 44100 = 0.02268 N f = f ′ ⋅ f s N {\displaystyle f=f'\cdot {\tfrac {f_{s}}{N}}} {\displaystyle f=f'\cdot {\tfrac {f_{s}}{N}}}
ω ′ = ω f s {\displaystyle \omega '={\tfrac {\omega }{f_{s}}}} {\displaystyle \omega '={\tfrac {\omega }{f_{s}}}}   [0, π] radians/sample 1000 × 2π / 44100 = 0.14250 ω = ω ′ ⋅ f s {\displaystyle \omega =\omega '\cdot f_{s}} {\displaystyle \omega =\omega '\cdot f_{s}}

See also

References

  1. Carlson, Gordon E. (1992). Signal and Linear System Analysis. Boston, MA: ©Houghton Mifflin Co. pp. 469, 490. ISBN 8170232384.
  2. Harris, Fredric J. (Jan 1978). "On the use of Windows for Harmonic Analysis with the Discrete Fourier Transform" (PDF). Proceedings of the IEEE. 66 (1): 51–83. Bibcode:1978IEEEP..66...51H. CiteSeerX 10.1.1.649.9880. doi:10.1109/PROC.1978.10837. S2CID 426548.
  3. Taboga, Marco (2021). "Discrete Fourier Transform - Frequencies", Lectures on matrix algebra. https://www.statlect.com/matrix-algebra/discrete-Fourier-transform-frequencies.